Torque free motion

The simulation displays (in the space frame on the left and in the body frame on the right) the evolution of a torque free ellipsoid around its center of mass. The Lagrangian is as follows:
L = ½ Ix ωx2Iy ωy2 + ½ Iz ωz2 ,
where the components of the angular velocity in the body frame are
ωx = φ' sin θ sin ψ + θ' cos ψ
ωy = φ' sin θ cos ψ - θ' sin ψ
ωz = φ' cos θ + ψ'
(we use ' for the time derivative). Reference: H. Goldstein, Ch. Poole and J. Safko, Classical Mechanics, 3rd edition, Addison-Wesley, San Francisco


Activities

  1. Press Start and get familiarized with the display options below the images.
  2. Let us check the Tennis Racket Theorem:



This is an English translation of the Basque original for a course on mechanics, oscillations and waves.
It requires Java 1.5 or newer and was created by Juan M. Aguirregabiria with Easy Java Simulations (Ejs) by Francisco Esquembre. I thank Wolfgang Christian and Francisco Esquembre for their help.